NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = B.Heusch Found 87 matches. 2002MA21 Phys.Rev. C65, 044006 (2002) F.M.Marques, M.Labiche, N.A.Orr, J.C.Angelique, L.Axelsson, B.Benoit, U.C.Bergmann, M.J.G.Borge, W.N.Catford, S.P.G.Chappell, N.M.Clarke, G.Costa, N.Curtis, A.D'Arrigo, E.de Goes Brennand, F.de Oliveira Santos, O.Dorvaux, G.Fazio, M.Freer, B.R.Fulton, G.Giardina, S.Grevy, D.Guillemaud-Mueller, F.Hanappe, B.Heusch, B.Jonson, C.Le Brun, S.Leenhardt, M.Lewitowicz, M.J.Lopez, K.Markenroth, A.C.Mueller, T.Nilsson, A.Ninane, G.Nyman, I.Piqueras, K.Riisager, M.G.Saint Laurent, F.Sarazin, S.M.Singer, O.Sorlin, L.Stuttge Detection of Neutron Clusters NUCLEAR REACTIONS C(14Be, nX), E=35 MeV/nucleon; C(11Li, nX), E=30 MeV/nucleon; C(15B, X), E=48 MeV/nucleon; measured En, (charged particle)n-, nn-coin, angular distributions; deduced possible neutron cluster formation.
doi: 10.1103/PhysRevC.65.044006
2001LA02 Phys.Rev.Lett. 86, 600 (2001) M.Labiche, N.A.Orr, F.M.Marques, J.C.Angelique, L.Axelsson, B.Benoit, U.C.Bergmann, M.J.G.Borge, W.N.Catford, S.P.G.Chappell, N.M.Clarke, G.Costa, N.Curtis, A.D'Arrigo, E.de Goes Brennand, O.Dorvaux, G.Fazio, M.Freer, B.R.Fulton, G.Giardina, S.Grevy, D.Guillemaud-Mueller, F.Hanappe, B.Heusch, K.L.Jones, B.Jonson, C.Le Brun, S.Leenhardt, M.Lewitowicz, M.J.Lopez, K.Markenroth, A.C.Mueller, T.Nilsson, A.Ninane, G.Nyman, F.de Oliveira, I.Piqueras, K.Riisager, M.G.Saint Laurent, F.Sarazin, S.M.Singer, O.Sorlin, L.Stuttge Halo Structure of 14Be NUCLEAR REACTIONS C, Pb(14Be, 2n12Be), E=35 MeV/nucleon; measured σ, neutron angular and momentum distributions, decay energy spectra. 14Be deduced halo features. Kinematically complete measurement, secondary beam from 18O fragmentation. Comparison with three-body model calculations.
doi: 10.1103/PhysRevLett.86.600
2001MA90 Phys.Rev. C64, 061301 (2001) F.M.Marques, M.Labiche, N.A.Orr, J.C.Angelique, L.Axelsson, B.Benoit, U.C.Bergmann, M.J.G.Borge, W.N.Catford, S.P.G.Chappell, N.M.Clarke, G.Costa, N.Curtis, A.D'Arrigo, E.de Goes Brennand, F.de Oliveira Santos, O.Dorvaux, G.Fazio, M.Freer, B.R.Fulton, G.Giardina, S.Grevy, D.Guillemaud-Mueller, F.Hanappe, B.Heusch, B.Jonson, C.Le Brun, S.Leenhardt, M.Lewitowicz, M.J.Lopez, K.Markenroth, A.C.Mueller, T.Nilsson, A.Ninane, G.Nyman, I.Piqueras, K.Riisager, M.G.Saint Laurent, F.Sarazin, S.M.Singer, O.Sorlin, L.Stuttge Three-Body Correlations in Borromean Halo Nuclei NUCLEAR REACTIONS C, Pb(14Be, 2n12Be), E=35 MeV/nucleon; analyzed particle spectra, invariant mass, three-body correlations. Intensity interferometry, Dalitz plots.
doi: 10.1103/PhysRevC.64.061301
2000MA12 Phys.Lett. 476B, 219 (2000) F.M.Marques, M.Labiche, N.A.Orr, J.C.Angelique, L.Axelsson, B.Benoit, U.C.Bergmann, M.J.G.Borge, W.N.Catford, S.P.G.Chappell, N.M.Clarke, G.Costa, N.Curtis, A.D'Arrigo, F.de Oliveira Santos, E.de Goes Brennand, O.Dorvaux, M.Freer, B.R.Fulton, G.Giardina, C.Gregori, S.Grevy, D.Guillemaud-Mueller, F.Hanappe, B.Heusch, B.Jonson, C.Le Brun, S.Leenhardt, M.Lewitowicz, M.J.Lopez, K.Markenroth, M.Motta, A.C.Mueller, T.Nilsson, A.Ninane, G.Nyman, I.Piqueras, K.Riisager, M.G.Saint Laurent, F.Sarazin, S.M.Singer, O.Sorlin, L.Stuttge Two-Neutron Interferometry as a Probe of the Nuclear Halo NUCLEAR REACTIONS Pb(6He, 2nα), E=50 MeV/nucleon; Pb(11Li, 2n9Li), E=30 MeV/nucleon; Pb(14Be, 2n12Be), E=35 MeV/nucleon; measured neutron spectra, (neutron)(neutron)(core)-coin; deduced correlation functions. 6He, 11Li, 14Be deduced radii, n-n separations. Secondary beams from 18O fragmentation.
doi: 10.1016/S0370-2693(00)00141-6
2000PA18 Phys.Rev. C61, 044614 (2000) M.Papa, F.Amorini, G.Cardella, M.Cavallaro, P.Figuera, A.Musumarra, G.Pappalardo, F.Rizzo, S.Romano, S.Tudisco, B.Heusch, Q.Wang, S.Si, J.Lu, W.Tian, P.Hu Fluctuations in the Excitation Functions of Dissipative Collisions Induced on the 27Al + 27Al System in the Laboratory Energy Range 114.2-123 MeV NUCLEAR REACTIONS 27Al(27Al, X), E=114.2-122.8 MeV; measured fragments σ(θ), energy, angular correlations; deduced energy coherence lengths, average angular velocity of intermediate dinuclear system. Partially overlapped molecular level model.
doi: 10.1103/PhysRevC.61.044614
1999DO07 Nucl.Phys. A651, 225 (1999) O.Dorvaux, L.Stuttge, F.Hanappe, G.Rudolf, G.Bizard, G.J.Costa, D.Durand, G.Guillaume, B.Heusch, A.Huck, C.Le Brun, F.R.Lecolley, S.Mouatassim, A.Ninane, B.Tamain, S.Tomasevic Study of the Excitation Energy Sharing and Dynamics using the Neutron Detector DeMoN in 86Kr + 165Ho Collisions at 60 A MeV NUCLEAR REACTIONS 165Ho(86Kr, X), E=60 MeV/nucleon; measured neutron spectra, multiplicity vs projectile-like-fragment charge; deduced intermediate velocity source, neck emission. Statistical, participant-spectator models.
doi: 10.1016/S0375-9474(99)00135-9
1999KE09 Europhys.Lett. 47, 552 (1999) A.Kelic, I.M.Itkis, I.V.Pokrovsky, E.V.Prokhorova, B.Benoit, G.Costa, L.Donadille, O.Dorvaux, E.De Goes Brennand, G.Guillaume, F.Hanappe, B.Heusch, A.Huck, M.G.Itkis, S.Jokic, N.A.Kondratev, E.M.Kozulin, Yu.Ts.Oganessian, G.Rudolf, A.Ya.Rusanov, L.Stuttge, D.Vorkapic, K.Yuasa-Nakagawa Prefission Neutron Multiplicities and the Fission Modes of 226Th NUCLEAR REACTIONS 208Pb(18O, X), E=78 MeV; measured neutron spectra, multiplicities, fragment mass distributions following compound nucleus fission; deduced relationship between fission modes and pre-, post-fission neutron multiplicity.
doi: 10.1209/epl/i1999-00424-4
1999WA26 Chin.Phys.Lett. 16, 876 (1999) Q.Wang, S.-L.Li, W.-D.Tian, P.-Y.Hu, J.Lu, F.Amorini, M.Cabibbo, G.Cardella, P.Figuere, A.Musumarra, M.Papa, G.Pappalardo, F.Rizzo, S.Romano, S.Tudisco, B.Heusch Non-Equilibrium Statistic Features in Dissipative Heavy Ion Collision 27Al +27Al NUCLEAR REACTIONS 27Al(27Al, X), E=114-127 MeV; measured σ(θ), σ(θ, E), energy autocorrelation; deduced non-equilibrium reaction mechanisms.
doi: 10.1088/0256-307X/16/12/007
1998CA02 Phys.Rev. C57, 731 (1998) Sl.Cavallaro, E.De Filippo, G.Lanzano, A.Pagano, M.L.Sperduto, R.Dayras, R.Legrain, E.Pollacco, C.Beck, B.Djerroud, R.M.Freeman, F.Haas, A.Hachem, B.Heusch, D.Mahboub, A.Morsad, R.Nouicer, S.J.Sanders Fusion and Binary-Decay Mechanisms in the 35Cl + 24Mg System at E/A ≈ 8 MeV NUCLEAR REACTIONS 24Mg(35Cl, X), E=282 MeV; measured fragments σ(E, Z, θ), fusion, binary mechanism σ; deduced partially-damped binary product decay times, reaction mechanism.
doi: 10.1103/PhysRevC.57.731
1998LA16 Phys.Rev. C58, 281 (1998) G.Lanzano, A.Pagano, G.Blancato, E.De Filippo, M.Geraci, R.Dayras, B.Berthier, F.Gadi-Dayras, R.Legrain, E.Pollacco, B.Heusch Inclusive Measurements of Light Charged Particles Emitted in the Reaction 40Ar + 27Al at 60A MeV NUCLEAR REACTIONS 27Al(40Ar, X), E=60 MeV/nucleon; measured Z=1, 2 fragments inclusive σ(E, θ); deduced source temperatures, anomalous α-particle abundance. Three-source model.
doi: 10.1103/PhysRevC.58.281
1997LE09 Nucl.Phys. A620, 327 (1997) F.R.Lecolley, B.Benoit, G.Bizard, G.Costa, O.Dorvaux, D.Durand, Y.El Masri, G.Guillaume, F.Gulminelli, F.Hanappe, B.Heusch, A.Huck, T.Keutgen, C.Le Brun, F.Lefebvres, M.Louvel, A.Ninane, R.Regimbart, G.Rudolf, J.C.Steckmeyer, L.Stuttge, B.Tamain, I.Tilquin Highest Temperatures Sustainable in Heavy Nuclei Produced in Ar + Au Collisions at 60A MeV NUCLEAR REACTIONS 197Au(Ar, X), E=60 MeV/nucleon; measured fragment kinematical characteristics, nn-coin; deduced total residue production σ, hot nuclei decay model. Microscopic transport model.
doi: 10.1016/S0375-9474(97)00066-3
1996FU17 Nucl.Phys. A607, 85 (1996) Y.Futami, K.Yuasa-Nakagawa, T.Nakagawa, S.M.Lee, K.Furutaka, K.Matsuda, K.Yoshida, S.C.Jeong, H.Fujiwara, T.Mizota, Y.Honjo, S.Tomita, B.Heusch, K.Ieki, J.Kasagi, W.Q.Shen, T.Matsuse Decay Mechanism of a Highly Excited Nucleus Produced in the Reaction 84Kr + 27Al at 10.6 MeV/Nucleon NUCLEAR REACTIONS 27Al(84Kr, X), E=10.6 MeV/nucleon; measured fragment production σ vs mass, σ(θ), light charged particle multiplicity.Statistical model calculation.
doi: 10.1016/S0375-9474(96)00223-0
1996MA25 Phys.Lett. 381B, 407 (1996) F.M.Marques, E.Liegard, N.A.Orr, J.C.Angelique, L.Axelsson, G.Bizard, W.N.Catford, N.M.Clarke, G.Costa, M.Freer, S.Grevy, D.Guillemaud-Mueller, G.J.Gyapong, F.Hanappe, P.G.Hansen, B.Heusch, B.Jonson, C.Le Brun, F.R.Lecolley, F.Lefebvres, M.Lewitowicz, G.Martinez, A.C.Mueller, T.Nilsson, A.Ninane, G.Nyman, B.Petersen, F.Pougheon, K.Riisager, M.G.Saint-Laurent, Y.Schutz, M.Smedberg, O.Sorlin, L.Stuttge, D.D.Warner Neutrons from the Breakup of 19C NUCLEAR REACTIONS Ta(19C, xn), E=30 MeV/nucleon; measured σ(θn). 19C deduced neutron halo. Core breakup reaction model.
doi: 10.1016/0370-2693(96)00617-X
1995CA06 Nucl.Phys. A583, 161c (1995) Sl.Cavallaro, C.Beck, E.Berthoumieux, R.Dayras, E.De Filippo, G.Di Natale, B.Djerroud, R.M.Freeman, A.Hachem, F.Haas, B.Heusch, G.Lanzano, R.Legrain, D.Mahboub, A.Morsad, A.Pagano, E.Pollacco, S.J.Sanders, M.L.Sperduto Origin and Decay-Properties of Binary Fragments Produced in the 35Cl + 24Mg Reaction at E/A ≈ 8 MeV/A NUCLEAR REACTIONS 24Mg(35Cl, X), E=260, 282.4 MeV; measured σ(fragment θ, E), (fragment)(fragment)(θ); deduced binary fragment origin, decay mechanisms.
doi: 10.1016/0375-9474(94)00725-3
1995MO36 Nucl.Instrum.Methods Phys.Res. A359, 530 (1995) S.Mouatassim, G.J.Costa, G.Guillaume, B.Heusch, A.Huck, M.Moszynski The Light Yield Response of NE213 Organic Scintillators to Charged Particles Resulting from Neutron Interactions NUCLEAR REACTIONS 12C(n, p), E ≈ 12-19 MeV; measured proton spectra; deduced proton, other particle light yields of detector. Organic NE213 scintillators, liquid NE213 cell, nγ-discrimination by charge integration method.
doi: 10.1016/0168-9002(95)00020-8
1994MO41 Nucl.Instrum.Methods Phys.Res. A343, 563 (1994) M.Moszynski, G.J.Costa, G.Guillaume, B.Heusch, A.Huck, S.Mouatassim, Y.El-Masri, P.Leleu, P.Lipnik, I.Tilquin, F.Hanappe, G.Bizard, D.Durand, J.Peter, B.Tamain, and the DEMON Collaboration Identification of Different Reaction Channels of High Energy Neutrons in Liquid Scintillators by the Pulse Shape Discrimination Method NUCLEAR REACTIONS 12C(n, d), (n, t), (n, 3He), (n, α), E=40, 56 MeV; measured σ in most cases; deduced reactions role in determining total efficiency of organic scintillators for high energy neutrons.
doi: 10.1016/0168-9002(94)90238-0
1993BE15 Phys.Rev. C47, 2093 (1993) C.Beck, B.Djerroud, F.Haas, R.M.Freeman, A.Hachem, B.Heusch, A.Morsad, M.Vuillet-A-Cilles, S.J.Sanders Asymmetric Fission of 47V Induced by the 23Na + 24Mg Reaction NUCLEAR REACTIONS 24Mg(23Na, X), (23Na, F), E=89.1 MeV; measured fragment total kinetic energy, σ vs charge. 47V deduced no entrance channel effects in fission. Other reactions data analyzed.
doi: 10.1103/PhysRevC.47.2093
1993BO18 Nuovo Cim. 106A 379 (1993) P.Boccaccio, P.K.Mwose, L.Vannucci, M.Bettiolo, R.A.Ricci, W.Augustyniak, I.Massa, G.Vannini, J.P.Coffin, P.Fintz, G.Guillaume, B.Heusch, F.Jundt, F.Rami, P.Wagner Three-Body Processes in the 32S + 45Sc Reaction at 5.6 MeV/u NUCLEAR REACTIONS 45Sc(32S, X), E=5.6 MeV/nucleon; measured (fragment)(fragment)-coin vs Z; deduced three-body production mechanism.
doi: 10.1007/BF02771453
1992BE34 Z.Phys. A343, 309 (1992) C.Beck, B.Djerroud, F.Hass, R.M.Freeman, A.Hachem, B.Heusch, A.Morsad, M.Youlal, Y.Abe, R.Dayras, J.P.Wieleczko, T.Matsuse, S.M.Lee Competition between the Fusion-Fission and Deep-Inelastic Orbiting Mechanisms in the 35Cl + 12C Reaction NUCLEAR REACTIONS 12C(35Cl, X), E=180, 200 MeV; measured evaporation residue σ(θ), fission like yields charge distributions, σ(θ), fragment spectra, (fragment)(fragment)-coin damped yields σ(E) for X=B-Mg; deduced fusion-fission rather than orbiting process evidence.
doi: 10.1007/BF01291530
1992LA10 Nucl.Instrum.Methods Phys.Res. A312, 515 (1992) G.Lanzano, A.Pagano, S.Urso, E.De Filippo, B.Berthier, J.L.Charvet, R.Dayras, R.Legrain, R.Lucas, C.Mazur, E.Pollacco, J.E.Sauvestre, C.Volant, C.Beck, B.Djerroud, B.Heusch Using BaF2 Crystals as Detectors of Light Charged Particles at Intermediate Energies NUCLEAR REACTIONS 27Al(40Ar, X), E=58 MeV/nucleon; measured bidimensional light charged particles fast vs total component spectra; deduced crystal light response. BaF2 crystal.
doi: 10.1016/0168-9002(92)90199-E
1992YU01 Phys.Lett. 283B, 185 (1992) K.Yuasa-Nakagawa, Y.H.Pu, S.C.Jeong, T.Mizota, Y.Futami, S.M.Lee, T.Nakagawa, B.Heusch, K.Ieki, T.Matsuse Complex Fragment Distributions in 84Kr + 27Al at E(lab) = 10.6 MeV/u NUCLEAR REACTIONS 27Al(84Kr, X), E=10.6 MeV/nucleon; measured complex fragment mass, charge distributions; deduced sequential decay mechanism features. Extended Hauser-Feshbach method.
doi: 10.1016/0370-2693(92)90005-O
1991MA30 Z.Phys. A339, 283 (1991) A.Malki, J.P.Coffin, G.Guillaume, F.Jundt, K.Krishan, F.Rami, P.Wagner, P.Fintz, M.Zahar, M.Gonin, B.Heusch, M.Ohta, B.Rastegar, F.Merchez, J.Mistretta, S.Kox Preequilibrium Versus Thermalized Light-Charged Particle Emissions in the 40Ar(1100 MeV) + 24Mg Reaction. Dynamical Calculations NUCLEAR REACTIONS 24Mg(40Ar, X), E=1100 MeV; measured fragment yield, (fragment)(fragment)(θ); deduced light particle emission processes separation. Light-heavy fragment coincidence, p, d, t, α particle detected.
doi: 10.1007/BF01284066
1991RA10 Phys.Rev. C44, 514 (1991) A.Ray, D.Shapira, J.Gomez del Campo, H.J.Kim, C.Beck, B.Djerroud, B.Heusch, D.Blumenthal, B.Shivakumar Compound Nucleus Origin of Back-Angle Yields in the 31P + 16O and 35Cl + 12C Reactions NUCLEAR REACTIONS 16O(31P, 16O), 16O(31P, 12C), E=135.6 MeV; measured σ(E, θ); deduced entrance channel dependence, orbiting yield. Comparison with other data.
doi: 10.1103/PhysRevC.44.514
1990LE22 Nucl.Phys. A519, 221c (1990) S.M.Lee, T.Nakagawa, B.Heusch, K.Yuasa-Nakagawa, Y.H.Pu, S.C.Jeong, H.Fujiwara, T.Mizota, K.Ieki, T.Sugimitsu, T.Matsuse Effects of Sequential Decay in Nuclear Element Distribution of Complex Fragment for 86Kr + 27Al at 10.6 MeV/u NUCLEAR REACTIONS 27Al(84Kr, X), E=10.6 MeV/nucleon; measured fragment production σ vs Z; deduced sequential decay evidence.
doi: 10.1016/0375-9474(90)90629-Z
1989BE37 Z.Phys. A334, 521 (1989) C.Beck, B.Djerroud, B.Heusch, R.Dayras, R.M.Freeman, F.Haas, A.Hachem, J.P.Wieleczko, M.Youlal Fusion-Fission in the 35Cl + 12C Reaction at E(lab) = 180 MeV NUCLEAR REACTIONS 12C(35Cl, X), E=180 MeV; measured (fragment)(fragment)-coin, fragment production σ vs Z; deduced reaction mechanism. Kinematical coincidence technique.
1989DA02 Phys.Rev.Lett. 62, 1017 (1989) R.Dayras, R.Coniglione, J.Barrette, B.Berthier, D.M.de Castro Rizzo, O.Cisse, F.Gadi, R.Legrain, M.C.Mermaz, H.Delagrange, B.Heusch, W.Mittig, G.Lanzano, A.Pagano Correlations between Projectilelike and Targetlike Fragments in the Reaction 27Al + 44-MeV/Nucleon 40Ar NUCLEAR REACTIONS 27Al(40Ar, X), E=44 MeV/nucleon; measured (fragment)(fragment)(θ); deduced reaction mechanism.
doi: 10.1103/PhysRevLett.62.1017
1988GO12 Phys.Rev. C38, 135 (1988) M.Gonin, J.P.Coffin, G.Guillaume, F.Jundt, P.Wagner, P.Fintz, B.Heusch, A.Malki, A.Fahli, S.Kox, F.Merchez, J.Mistretta Preequilibrium Emission and Incomplete Fusion of Low and Medium Mass Heavy Ion Systems NUCLEAR REACTIONS 45Sc(40Ar, X), 24Mg(40Ar, X), 13C(40Ar, X), E=1100 MeV; measured fragment velocity, light particle (p, d, t, α) energy, σ(θ), σ(E, A); deduced projectile linear momentum transfer, compound nucleus excitation energy, temperature, entrance channel asymmetry dependence, incomplete fusion, pre-equilibrium emission properties.
doi: 10.1103/PhysRevC.38.135
1988VA25 Europhys.Lett. 7, 311 (1988) G.Vannini, I.Massa, L.Lavagnini, P.Boccaccio, L.Vannucci, R.A.Ricci, I.Iori, J.P.Coffin, P.Fintz, M.Gonin, G.Guillaume, B.Heusch, F.Jundt, A.Malki, F.Rami, P.Wagner Experimental Evidence of Three-Body Process in the 32S + 59Co Reaction at 5.6 MeV/u NUCLEAR REACTIONS 59Co(32S, X), E=180 MeV; measured (fragment)(fragment)-coin; deduced reaction mechanism.
doi: 10.1209/0295-5075/7/4/005
1987FA02 Z.Phys. A326, 169 (1987) A.Fahli, J.P.Coffin, G.Guillaume, B.Heusch, F.Jundt, F.Rami, P.Wagner, P.Fintz, A.J.Cole, S.Kox, Y.Schutz, N.Cindro Light Charged Particle Emission in 40Ar Induced Reactions on 68Zn at 14.6, 19.6 and 35 MeV/Nucleon NUCLEAR REACTIONS 68Zn(40Ar, X), E=14.6, 19.6, 35 MeV/nucleon; measured σ(fragment θ), σ(fragment θ, E), for X=p, d, t, 3,4He, 6,7Li. Enriched target, telescope system. Preequilibrium emission, moving source, coalescence models.
1987HE12 Fizika(Zagreb) 19, Supplement 1, 57 (1987) B.Heusch, J.Barrette, B.Berthier, D.M.de Castro Rizzo, O.Cisse, R.Dayras, F.Dayras-Gadi, B.Faure, R.Legrain, M.Mermaz, E.Pollacco, J.P.Wieleczko, H.Delagrange, W.Mittig, R.Coniglione, G.Lanzano, A.Pagano Projectile-Like-Target-Like Fragment Correlations in Peripheral Collisions of 40Ar on 27Al and (nat)Ag Targets at GANIL Energies NUCLEAR REACTIONS Ag(40Ar, X), E=30, 60 MeV/nucleon; measured (projectile-like fragment)(target-like fragment)-coin; deduced abrasion-ablation mechanism dominance.
1987RA10 Z.Phys. A327, 207 (1987) F.Rami, A.Fahli, J.P.Coffin, G.Guillaume, B.Heusch, F.Jundt, P.Wagner, P.Fintz, S.Kox, Y.Schutz, M.C.Mermaz Origin of Projectile-Like Fragments from 40Ar + 68Zn Collisions between 15 and 35 MeV/Nucleon: Direct transfer of nucleons and projectile fragmentation NUCLEAR REACTIONS 68Zn(40Ar, X), E=14.6, 19.6, 27.6, 35 MeV/nucleon; measured σ(fragment θ, E), σ(fragment θ), σ(fragment Z); deduced fragment velocities, linear momentum distribution widths. Enriched target, tof, ΔE-E telescope.
1987SU07 Phys.Rev. C36, 181 (1987) T.Suomijarvi, B.Berthier, R.Lucas, M.C.Mermaz, J.P.Coffin, G.Guillaume, B.Heusch, F.Jundt, F.Rami Correlated Fluctuations in the 89Y(19F, x)y Excitation Functions NUCLEAR REACTIONS 89Y(19F, X), E=135-143.25 MeV; measured σ(θ) vs E; deduced coherence width, fragment T1/2, quasimolecular configurations.
doi: 10.1103/PhysRevC.36.181
1986BA34 Nucl.Phys. A456, 489 (1986) D.Bangert, F.Busch, B.Kohlmeyer, F.Puhlhofer, H.Freiesleben, B.Heusch, K.D.Hildenbrand, W.F.W.Schneider, D.Schull Symmetric Fragmentation in the System 132Xe + 56Fe at 5.0, 5.7 and 8.5 MeV/u Beam Energy NUCLEAR REACTIONS 56Fe(132Xe, X), E=5, 5.7, 8.5 MeV/nucleon; measured σ(fragment θ); deduced fission, capture σ(E), compound nucleus formation mechanisms.
doi: 10.1016/0375-9474(86)90407-0
1986DA20 Nucl.Phys. A460, 299 (1986) R.Dayras, A.Pagano, J.Barrette, B.Berthier, D.M.De Castro Rizzo, E.Chavez, O.Cisse, R.Legrain, M.C.Mermaz, E.C.Pollacco, H.Delagrange, W.Mittig, B.Heusch, R.Coniglione, G.Lanzano, A.Palmeri Peripheral Interactions for 44 MeV/u 49Ar on 27Al and Ti(nat) Targets NUCLEAR REACTIONS 27Al, Ti(40Ar, X), E=1760 MeV; measured σ(fragment E, θ). Tof, telescope spectrometers, solid state detectors, natural targets. Abrasion model calculations.
doi: 10.1016/0375-9474(86)90128-4
1986FA05 Phys.Rev. C34, 161 (1986) A.Fahli, J.P.Coffin, G.Guillaume, B.Heusch, F.Jundt, F.Rami, P.Wagner, P.Fintz, A.J.Cole, S.Kox, Y.Schutz Incomplete Fusion in the 40Ar + 68Zn Reaction: Trends and limits NUCLEAR REACTIONS 68Zn(40Ar, X), E=14.6, 19.6, 27.6, 35 MeV/nucleon; measured σ(fragment θ), fragment mass vs velocity; deduced fusion σ(E), reaction mechanism.
doi: 10.1103/PhysRevC.34.161
1986ME06 Nucl.Phys. A456, 186 (1986) M.C.Mermaz, T.Suomijarvi, R.Lucas, B.Berthier, J.Matuszek, J.P.Coffin, G.Guillaume, B.Heusch, F.Jundt, F.Rami From Quasi-Elastic to Quasi-Compound Nucleus Reactions Induced by 140 MeV 19F Beam bombarding 89Y Target Nuclei NUCLEAR REACTIONS 89Y(19F, X), E=140 MeV; measured fragment mass, charge distributions; deduced quasielastic, deep inelastic, compound nucleus-like production σ. Natural targets, time-of-flight, telescope spectrometers.
doi: 10.1016/0375-9474(86)90373-8
1985BE37 Nucl.Phys. A443, 157 (1985) C.Beck, R.M.Freeman, F.Haas, B.Heusch, J.J.Kolata Role of the Valence Neutron in the 12C + 17O and 13C + 16O Collisions NUCLEAR REACTIONS, ICPND 12C(17O, X), 13C(16O, X), E=20-70 MeV; measured γ-ray yields of reaction products; deduced resonant behavior, Landau-Zener effect. Hauser-Feshbach analysis.
doi: 10.1016/0375-9474(85)90326-4
1985BE40 Nucl.Phys. A442, 320 (1985) C.Beck, F.Haas, R.M.Freeman, B.Heusch, J.P.Coffin, G.Guillaume, F.Rami, P.Wagner Comparison of Cross Sections for C + O Reactions in the Second Regime of Complete Fusion NUCLEAR REACTIONS, ICPND 12C(18O, X), E=32-140 MeV; 13C(17O, X), E=54-140 MeV; 12C(16O, X), E=62-150 MeV; 16O(12C, X), E=46.5-112.5 MeV; measured σ(fragment θ, E) for fragment Z=3-14, fusion σ(E); deduced critical, grazing angular momenta. 28Si deduced possible superdeformation. Statistical, complete fusion model predictions.
doi: 10.1016/0375-9474(85)90148-4
1985CO27 Nucl.Phys. A447, 95c (1985) R.Coniglione, G.Lanzano, A.Pagano, J.Barrette, B.Berthier, D.M.C.Castro Rizzo, O.Cisse, R.Dayras, R.Legrain, M.C.Mermaz, H.Delagrange, W.Mittig, B.Heusch Projectile and Target Fragment Correlations in the Reaction 40Ar + 27Al at E(Lab)/A = 44 MeV NUCLEAR REACTIONS 27Al(40Ar, X), E=44 MeV/nucleon; measured projectile, target fragment mass correlation, (fragment)(fragment)(θ); deduced two abraded fragment correlation. Abrasion model.
doi: 10.1016/0375-9474(86)90599-3
1985HE17 Z.Phys. A322, 309 (1985) B.Heusch, H.Freiesleben, W.F.W.Schneider, B.Kohlmeyer, H.Stege, F.Puhlhofer A Fast-Fission Component with Small Mass Drift in the Reaction 84Kr + 27Al at E(lab) = 5.9 MeV/u NUCLEAR REACTIONS 27Al(84Kr, X), E=5.94 MeV/nucleon; measured σ(fragment θ) for fragment Z=10-41; deduced total, reaction, deep inelastic, quasielastic, evaporation, fast fission σ, maximum (L).
doi: 10.1007/BF01411896
1985ME08 Phys.Rev. C31, 1972 (1985) M.C.Mermaz, F.Rami, J.P.Coffin, G.Guillaume, B.Heusch, P.Wagner, A.Fahli, P.Fintz Direct Surface Transfer Reactions Induced by a 1102 MeV 40Ar Beam on 68Zn Target Nucleus NUCLEAR REACTIONS 68Zn(40Ar, X), E=1102 MeV; measured σ(fragment θ, E) for X=42,41Ca, 36,37Cl, 39K; deduced level densities, diffraction model parameters.
doi: 10.1103/PhysRevC.31.1972
1985ME11 Nucl.Phys. A441, 129 (1985) M.C.Mermaz, R.Dayras, J.Barrette, B.Berthier, D.M.De Castro Rizzo, O.Cisse, R.Legrain, A.Pagano, E.Pollacco, H.Delagrange, W.Mittig, B.Heusch, G.Lanzano, A.Palmeri Direct Surface-Transfer Reaction to the Continuum States Induced by a 1760 MeV 40Ar Beam on 27Al and (nat)Ti Target Nuclei NUCLEAR REACTIONS 27Al, Ti(40Ar, X), E=1760 MeV; measured σ(fragment E, θ) for X=41,42Ca, 39,40K, 36,37,38,39,41Ar, 36S; deduced model parameters. 27Al, Ti deduced level densities. Natural targets. Diffraction model.
doi: 10.1016/0375-9474(85)90171-X
1985RA23 Nucl.Phys. A444, 325 (1985) F.Rami, J.P.Coffin, G.Guillaume, B.Heusch, P.Wagner, A.Fahli, P.Fintz Study of the 40Ar + 68Zn Reaction at 27.6 MeV/Nucleon NUCLEAR REACTIONS 68Zn(40Ar, X), E=1102 MeV; measured fragment σ(θ), σ(E, Z, A); deduced reaction σ, dominant reaction mechanisms. Time-of-flight, telescope spectrometers, solid-state detectors. Enriched target.
doi: 10.1016/0375-9474(85)90353-7
1985SU06 Z.Phys. A321, 531 (1985) T.Suomijarvi, R.Lucas, M.C.Mermaz, J.-P.Coffin, G.Guillaume, B.Heusch, F.Jundt, F.Rami Lifetime-Parameters for Quasi Elastic and Deep Inelastic Collisions Extracted from Complete Angular Distributions of 89Y(19F, x)y Reactions NUCLEAR REACTIONS 89Y(19F, X), E=140 MeV; measured σ(fragment θ), σ(fragment E) for Z=3-11; deduced reaction mechanisms, dinuclear system T1/2.
1984BE22 Phys.Rev. C29, 1942 (1984) C.Beck, F.Haas, R.M.Freeman, B.Heusch, J.P.Coffin, G.Guillaume, F.Rami, P.Wagner Fusion Cross Sections of the 12C + 16O Reaction at E(16O) up to 150 MeV NUCLEAR REACTIONS, ICPND 12C(16O, X), 16O(12C, X), E(cm)=26.6, 34.3, 42.9, 53.6, 64.3 MeV; measured evaporation residue yields; deduced fusion σ(E), critical, grazing (L).
doi: 10.1103/PhysRevC.29.1942
1984CO14 Phys.Rev. C30, 539 (1984) J.P.Coffin, G.Guillaume, A.Fahli, F.Rami, B.Heusch, P.Wagner, P.Engelstein, P.Fintz, N.Cindro Transitional Dissipative Mechanism in the 32S + 59Co Reaction NUCLEAR REACTIONS 59Co(32S, X), (32S, F), E=128, 143, 158, 178, 198 MeV; measured fission, evaporation residue fragment energy, mass distributions, σ(E), σ(fragment θ, A); deduced fusion σ, fission mechanism.
doi: 10.1103/PhysRevC.30.539
1984DE39 Nucl.Phys. A429, 173 (1984) H.Delagrange, A.Benachou, F.Hubert, Y.Llabador, B.Heusch, J.P.Coffin, P.Engelstein, P.Fintz, G.Guillaume Statistical Decay of 193Au, 194Hg and 198Hg Compound Nuclei NUCLEAR REACTIONS, ICPND 181Ta(12C, F), E=60-110 MeV; 182W(12C, F), E=70-130 MeV; 186W(12C, F), E=80-100 MeV; measured fission σ(E). 181Ta(12C, X), E=105 MeV; measured σ(fragment θ, E), σ(fragment θ, mass). 182W(12C, X), E=98.7 MeV; measured evaporation residue σ(θ). 181Ta, 182,186W(12C, α), E=80, 98.7 MeV; measured σ; deduced fission mechanism, fusion σ. Statistical decay.
doi: 10.1016/0375-9474(84)90154-4
1984RA12 Z.Phys. A318, 239 (1984) F.Rami, J.P.Coffin, G.Guillaume, B.Heusch, P.Wagner, A.Fahli, P.Fintz Few Nucleon Transfer Versus Fragmentation in the Production of Projectile-Like Fragments in the 40Ar + 68Zn Reaction at 27.6 MeV/Nucleon NUCLEAR REACTIONS 68Zn(40Ar, X), E=27.6 MeV/nucleon; measured fragment velocity, momentum width, isotope distributions; deduced fragmentation process, nucleon transfer, damped collision roles.
doi: 10.1007/BF01413475
1983FR17 Phys.Rev. C28, 437 (1983) R.M.Freeman, C.Beck, F.Haas, B.Heusch, J.J.Kolata Resonant Effects in the 13C + 17O Reaction NUCLEAR REACTIONS, ICPND 13C(17O, 17O'), E=35-60 MeV; measured γ yield vs E. 17O transition deduced single particle character. Nuclear Landau-Zener effect.
doi: 10.1103/PhysRevC.28.437
1983HE11 Z.Phys. A312, 109 (1983) B.Heusch, J.P.Coffin, P.Engelstein, G.Guillaume, F.Rami, D.Guerreau, J.Peter, Z.Zheng Fissionlike Exit Channel in the 5.8 MeV/u 84Kr on 24Mg Reaction NUCLEAR REACTIONS 24Mg(84Kr, X), E=490 MeV; measured σ(fragment θ, Z); deduced σ vs Z, fission type reaction entrance channel mass asymmetry, deep inelastic components. Extra push, Glas-Mosel, fusion-evaporation models.
doi: 10.1007/BF01411667
1982GU19 Phys.Rev. C26, 2458 (1982) G.Guillaume, J.P.Coffin, F.Rami, P.Engelstein, B.Heusch, P.Wagner, P.Fintz, J.Barrette, H.E.Wegner Fissionlike Component in the 32S + 76Ge Reaction NUCLEAR REACTIONS 76Ge(32S, 32S), (32S, X), (32S, F), E=3.4-7 MeV/nucleon; measured fission σ(E), fragment mass, energy distributions, σ(elastic), σ(fusion), σ(evaporation residue) vs E; deduced reaction mechanism. Enriched target, tof spectrometer.
doi: 10.1103/PhysRevC.26.2458
1982HE07 Phys.Rev. C26, 542 (1982) B.Heusch, C.Beck, J.P.Coffin, P.Engelstein, R.M.Freeman, G.Guillaume, F.Haas, P.Wagner Entrance Channel Effects for Complete Fusion of O + C Isotopes NUCLEAR REACTIONS, ICPND 12C(18O, 18O), (18O, X), E=32-140 MeV; 13C(17O, 17O), (17O, X), E=54-140 MeV; 14C(16O, 16O), (16O, X), E(cm)=10-60 MeV; measured σ(θ), evaporation σ vs E; deduced entrance channel effects, fusion evaporation. Tof fragment identification. Statistical, macroscopic models.
doi: 10.1103/PhysRevC.26.542
1981BE64 Fizika(Zagreb) 13, Suppl.No.1, 27 (1981) C.Beck, R.M.Freeman, F.Haas, B.Heusch, H.Bohn, K.A.Eberhard, U.Kaufl, H.Puchta, T.Senftleben, W.Trautmann Resonant Structure in the Reaction Channels of 14C + 14C NUCLEAR REACTIONS 14C(14C, 14C'), (14C, xn), (14C, xnα), E(cm)=12.5-32.5 MeV; measured σ(E), production σ(E) for 25Mg, 22Ne, Ne, 15C; deduced channel correlated structure. 28Mg deduced possible quasimolecular resonances.
1981FR23 Phys.Rev. C24, 2390 (1981) R.M.Freeman, C.Beck, F.Haas, B.Heusch, H.Bohn, U.Kaufl, K.A.Eberhard, H.Puchta, T.Senftleben, W.Trautmann Structure in the Reaction Channels of 14C + 14C NUCLEAR REACTIONS 14C(14C, 14C'), (14C, X), E(cm)=12.5-32.5 MeV; measured Eγ, Iγ; deduced production σ(E) for 15C, 21,22,23Ne, 25Mg, channel correlated resonance structure. Enriched target.
doi: 10.1103/PhysRevC.24.2390
1981GU16 Fizika(Zagreb) 13, Suppl.No.1, 66 (1981) G.Guillaume, F.Rami, J.P.Coffin, P.Engelstein, P.Fintz, B.Heusch, P.Wagner Symmetric Fragmentation of the 32S + 76Ge System Studied between 4.9 and 7.0 MeV/u NUCLEAR REACTIONS, Fission 76Ge(32S, X), (32S, F), E=158, 178, 198, 218, 225 MeV; measured absolute σ(fusion), σ(evaporation), σ(reaction) vs E. 108Cd deduced symmetric fission, deep inelastic, relaxed component process separation. Tof spectrometer.
1981HE08 Phys.Rev. C23, 1527 (1981) B.Heusch, C.Beck, J.P.Coffin, R.M.Freeman, A.Gallmann, F.Haas, F.Rami, P.Wagner, D.E.Alburger Systematics of Carbon + Carbon Fusion-Evaporation Reactions NUCLEAR REACTIONS 13C(13C, X), E=30-60 MeV; 12C, 13C, 14C(12C, X), E=40 MeV; measured σ(fragment θ, Z, mass), fusion-evaporation yields for 16,17,18O, 20,21,22Ne, 24,25Mg, 22,23,24Na, 19,20,21F. Enriched targets, tof fragment charge identification. Statistical particle evaporation calculations.
doi: 10.1103/PhysRevC.23.1527
1981KO07 Phys.Rev. C23, 1056 (1981) J.J.Kolata, C.Beck, R.M.Freeman, F.Haas, B.Heusch Structure in the 14C + 16O Reaction Cross Sections NUCLEAR REACTIONS 14C(16O, 22Ne), (16O, 18O), (16O, 17O), (16O, 15N), (16O, 14C), E(cm)=16.34 MeV; measured production σ; deduced resonance structure. 30Si deduced resonances, J, π, moment of inertia of crossing band.
doi: 10.1103/PhysRevC.23.1056
1980HE11 J.Phys.(Paris), Colloq.C-10, 229 (1980) B.Heusch, C.Beck, J.P.Coffin, R.M.Freeman, A.Gallmann, F.Haas, F.Rami, P.Wagner, D.E.Alburger The 18O + 12C Fusion-Evaporation Reaction NUCLEAR REACTIONS 12C(18O, X), E=32-100 MeV; 14C(16O, X), E=50 MeV; 12C(16O, X), E not given; measured σ(fragment mass, E); deduced production σ for Si, Al, Mg, Na, Ne. 30Si deduced no resonance structure in fusion channels. Statistical Hauser-Feshach calculations, Monte Carlo technique. Tof.
1980KO02 Phys.Rev. C21, 579 (1980) J.J.Kolata, R.M.Freeman, F.Hass, B.Heusch, A.Gallmann Reaction Cross Sections for 12C + 12C NUCLEAR REACTIONS 12C(12C, X), E(cm)=14-31 MeV; measured production σ(E) for 22,23Na, 19,20,21,22Ne, 18,19F, 16O, 12C; deduced fusion σ, inelastic σ, 3α evaporation σ. 24Mg deduced fusion L trajectory.
doi: 10.1103/PhysRevC.21.579
1980OE02 Phys.Rev. C22, 546 (1980) H.Oeschler, H.Freiesleben, K.D.Hildenbrand, P.Engelstein, J.P.Coffin, B.Heusch, P.Wagner Compound Nucleus Fission at High Angular Momentum Studied in the Reaction 132Xe+30Si NUCLEAR REACTIONS 132Xe(30Si, X), E=5.4-8.2 MeV/nucleon; measured σ(fragment mass, Z, θ), fission σ(E), evaporation residue σ(E), fusion σ(E); deduced nonequilibrium effects in compound nuclear fission. Enriched target, tof.
doi: 10.1103/PhysRevC.22.546
1979FR08 Phys.Rev. C20, 569 (1979) R.M.Freeman, F.Haas, B.Heusch, S.M.Lee Comparison of the γ-Ray Yield Functions for the 12C + 24Mg and 16O + 28Si Reactions NUCLEAR REACTIONS 12C(24Mg, X), E=45-71 MeV; 16O(28Si, X), E=55-96 MeV; measured Iγ(E), nγ-coin; deduced reaction mechanism. 34Cl, 34S, 31P, 28Si, 28Mg, 38Ar, 41,42Ca, 39K deduced production σ(E). Natural C, O targets.
doi: 10.1103/PhysRevC.20.569
1979KO03 Phys.Rev. C19, 408 (1979) J.J.Kolata, R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Reaction Cross Sections for 16O + 12C NUCLEAR REACTIONS 12C(16O, X), E(cm)=17-28 MeV; measured σ(E, production). Evaporation model analysis of nuclide distributions. Correlation analysis of fluctuations.
doi: 10.1103/PhysRevC.19.408
1979KO15 Phys.Rev. C19, 2237 (1979) J.J.Kolata, R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Gross and Intermediate-Width Structure in the Interaction of 16O with 16O NUCLEAR REACTIONS 16O(16O, X), E(cm)=12-40 MeV; measured production σ for 20Ne, 23Na, 27,28,29,30Si, 30,31P, 26,27Al, 24,26Mg; deduced total σ(fusion), barrier height, critical parameters, normalizations. Evaporation model, optical model analysis.
doi: 10.1103/PhysRevC.19.2237
1978BA76 Fizika, Suppl. 10, 11 (1978) P.Baumann, A.M.Bergdolt, G.Bergdolt, R.M.Freeman, F.Haas, B.Heusch, A.Huck, G.Walter Study of High Spin States in 30P and 32P NUCLEAR REACTIONS 16O(16O, np), E=42 MeV; 18O(16O, np), E=35 MeV; measured nγ-, γγ-coin, Eγ, Iγ. 27Al(α, n), E=14.6 MeV; measured RDM. 30P deduced levels, J, π, T1/2, B(λ). 32P deduced levels, J, π, T1/2.
1978CO07 Phys.Rev. C17, 1607 (1978) J.P.Coffin, P.Engelstein, A.Gallmann, B.Heusch, P.Wagner, H.E.Wegner 18O + 12C and 18O + 13C Fusion-Evaporation Reactions NUCLEAR REACTIONS 12,13C(18O, X), E=100 MeV; measured fusion σ(A, Z).
doi: 10.1103/PhysRevC.17.1607
1978HE20 Z.Phys. A288, 391 (1978) B.Heusch, C.Volant, H.Freiesleben, R.P.Chestnut, K.D.Hildenbrand, F.Puhlhofer, W.F.W.Schneider, B.Kohlmeyer, W.Pfeffer The Reaction Mechanism in the System 132Xe + 56Fe at 5.73 MeV/u: Evidence for a New Type of Strongly Damped Collisions NUCLEAR REACTIONS 56Fe(132Xe, X), E=5.73 MeV/nucleon; measured σ(E, θ) for target-, projectile-like fragments; deduced evidence for a new type of damped collision.
doi: 10.1007/BF01417723
1977DI17 Aust.J.Phys. 30, 417 (1977) A Study of the 42Ca(p, γ)43Sc Reaction NUCLEAR REACTIONS 42Ca(p, γ), E < 2.75 MeV; measured Eγ, Iγ, γ(θ). 43Sc deduced resonances, levels, J, π, γ-branching.
doi: 10.1071/PH770417
1977HA11 Nucl.Phys. A279, 237 (1977) F.Haas, R.M.Freeman, B.Heusch, A.Gallmann Structure en Bande du Noyau 22Na: le Premier Niveau Jπ = 6+ NUCLEAR REACTIONS 19F(α, n), E=7.825, 8.225 MeV; measured n-γ(θ), Doppler shift attenuation. 22Na levels deduced J, π, branching ratios, δ, T1/2, transition strengths.
doi: 10.1016/0375-9474(77)90226-3
1977HE04 Phys.Rev. C15, 1196 (1977) B.Heusch, F.Haas, R.M.Freeman, A.Gallmann Experimental Study of the 12C(3He, p)14N Reaction Mechanism between 11 And 20 MeV Bombarding Energy NUCLEAR REACTIONS 12C(3He, pγ), E=11-20 MeV; measured pγ(θ); deduced reaction mechanism, nuclear alignments.
doi: 10.1103/PhysRevC.15.1196
1977KO16 Phys.Rev. C16, 891 (1977) J.J.Kolata, R.C.Fuller, R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Reaction Cross Sections for 16O + 16O NUCLEAR REACTIONS 16O(16O, X), E(cm)=12.5-30.5 MeV; measured σ(A) for production of A=16-31 reaction products; deduced broad shape resonances.
doi: 10.1103/PhysRevC.16.891
1976DA14 J.Phys.(Paris) 37, 819 (1976) Proprietes des Niveaux de 61Cu et 63Cu par un Modele a Couplage Coeur-Particule NUCLEAR STRUCTURE 61,63Cu; calculated levels, S, T1/2, γ-branching, δ, B(λ).
doi: 10.1051/jphys:01976003707-8081900
1976FR09 Nucl.Phys. A261, 471 (1976) R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Largeurs de Transitions Gamma du Niveau a 2788 keV de 21Ne NUCLEAR REACTIONS 18O(α, n), E=4.7 MeV; measured Iγ, γγ(θ), recoil distance. 21Ne deduced branching ratios, δ, T1/2, transition strengths.
doi: 10.1016/0375-9474(76)90160-3
1976FR19 Phys.Rev. C14, 2006 (1976) R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Strong Isoscalar M2 Transition in 22Na NUCLEAR REACTIONS 19F(α, nγ), E=5.5 MeV; measured n, γ spectra. 22Na level deduced γ-branching.
doi: 10.1103/PhysRevC.14.2006
1976KO24 Phys.Lett. 65B, 333 (1976) J.J.Kolata, R.M.Freeman, F.Haas, B.Heusch, A.Gallmann On the Fusion Cross Section for 16O + 12C NUCLEAR REACTIONS 12C(16O, X), E=40-65 MeV; measured total fusion σ(E).
doi: 10.1016/0370-2693(76)90235-5
1973FR18 Phys.Rev. C8, 2182 (1973) R.M.Freeman, F.Haas, B.Heusch, J.Fernandez Castillo, J.W.Olness, A.Gallmann Rotational Band Structure of 22Na. II. Neutron-Gamma Coincidence Measurements NUCLEAR REACTIONS 19F(α, nγ), E=11 MeV; measured nγ(θ, t), DSA, γγ(θ). 22Na levels deduced T1/2, quadrupole moment.
doi: 10.1103/PhysRevC.8.2182
1973HA40 Nucl.Phys. A211, 289 (1973) F.Haas, R.M.Freeman, B.Heusch, S.Kohmoto, A.Gallmann Vies Moyennes dans 14N NUCLEAR REACTIONS 12C(3He, pγ), E=5.54 MeV; measured Eγ, DSA, σ(Ep, Eγ, θ(pγ)). 14N deduced levels, T1/2. Natural 12C targets self-supporting or on Ni backing.
doi: 10.1016/0375-9474(73)90720-3
1973HE09 Phys.Rev. C7, 1810 (1973) Study of the 12C(h, p)14N Reaction Mechanism by a Systematic Use of the p-γ Angular-Correlation Method NUCLEAR REACTIONS 12C(3He, pγ), E=3-11 MeV; measured σ(E, θ), pγ(θ). 14N levels deduced alignment.
doi: 10.1103/PhysRevC.7.1810
1971DA22 Nucl.Phys. A173, 49 (1971) R.Dayras, M.Toulemonde, B.Cujec, B.Heusch, J.N.Mo, I.M.Szoghy Mesures de Correlations Angulaires et de Vies Moyennes dans 57Co NUCLEAR REACTIONS 54Fe(α, pγ), E=9.86, 10.02, 10.40 MeV; measured σ(E;Ep, Eγ, θ(pγ)), Iγ, Doppler-shift attenuation. 57Co deduced γ-branching, J, γ-mixing, mean T1/2. Enriched targets.
doi: 10.1016/0375-9474(71)90747-0
1971HE14 Nucl.Phys. A169, 145 (1971) B.Heusch, B.Cujec, R.Dayras, J.N.Mo, I.M.Szoghy Etude du Noyau 61Cu par la Reaction 58Ni(α, pγ)61Cu NUCLEAR REACTIONS 58Ni(α, pγ); measured σ(E;Ep, Eγ, θ(pγ)). 61Cu deduced levels, J, π, γ-mixing, branching ratios. Isotopic 58Ni, self-supporting targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(71)90568-9
1971HE17 Nucl.Phys. A172, 395 (1971) Mesures de Vies Moyennes dans le Noyau 61Cu NUCLEAR REACTIONS 58Ni(α, pγ), E=10.01 MeV; measured Doppler-shift attenuation. 61Cu deduced T1/2, γ-width(M1), γ-width(E2). Enriched target.
doi: 10.1016/0375-9474(71)90721-4
1970GA01 Nucl.Phys. A143, 326 (1970) A.Gallmann, G.Frick, B.Heusch, F.Haas, E.K.Warburton Mesures de Vies Moyennes dans 13C et 10B par la Methode du Parcours de Recul NUCLEAR REACTIONS 10B(α, pγ), E = 1.96 MeV; 7Li(α, nγ), E = 8.95 MeV; measured Eγ(θ(γ) = 0°), Doppler shift, recoil distance. 13C, 10B deduced levels, T1/2. Enriched 10B, natural Li targets.
doi: 10.1016/0375-9474(70)90567-1
1970GA09 Can.J.Phys. 48, 1595 (1970) A.Gallman, F.Haas, N.Balaux, B.Heusch, M.Toulemonde Mesures de Vies Moyennes dans 12B, 14N et 16O NUCLEAR REACTIONS 11B(d, pγ), E=2.1 MeV; 19F(p, αγ), E=4.1 MeV; 12C(3He, pγ), E=4 MeV; measured Doppler-shift attenuation. 12B, 14N, 16O levels deduced T1/2.
doi: 10.1139/p70-201
1970HA52 Nucl.Phys. A156, 385 (1970) F.Haas, B.Heusch, G.Frick, A.Gallmann, D.E.Alburger Vies Moyennes des Niveaux de 3.79 MeV de 30Si et 0.709 MeV de 30P NUCLEAR REACTIONS 27Al(α, pγ), E=4.60 MeV; 27Al(α, nγ), E=8.50 MeV; measured Eγ, recoil distance. 30Si, 30P levels deduced T1/2.
doi: 10.1016/0375-9474(70)90149-1
1969GA16 Rev.Phys.Appl. 4, 216 (1969) A.Gallmann, F.Haas, B.Heusch, M.Toulemonde Mesures de Vies Moyennes par Effet Doppler NUCLEAR REACTIONS 11B(d, p), E=2.1 MeV; 12C(3He, p), E=4 MeV; measured Doppler shift attenuation. 12B, 14N levels deduced T1/2. Ge(Li) detector.
doi: 10.1051/rphysap:0196900402021601
1969HA49 Phys.Rev. 188, 1625 (1969) F.Haas, B.Heusch, A.Gallmann, D.A.Bromley Experimental Investigations of the C12(h, p)N14 Reaction Mechanism NUCLEAR REACTIONS 12C(3He, pγ), E=4.6-11 MeV; measured σ(E;θ(p), θ(pγ)); deduced heavy-particle direct stripping. 15O deduced resonances. 14N deduced level population.
doi: 10.1103/PhysRev.188.1625
1967GA12 Phys.Rev. 164, 1257 (1967) Study of Unbound Levels in N14 by the C12(He3, pγ)N14 Reaction NUCLEAR STRUCTURE 12C, 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.164.1257
1967GO07 Phys.Rev. 155, 1119 (1967) S.Gorodetzky, R.M.Freeman, A.Gallmann, F.Haas, B.Heusch Angular-Correlation Studies of the Reactions O16(He3, Pγ)F18 and O16(He3, αγ)O15 NUCLEAR STRUCTURE 18F, 16O, 15O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.155.1119
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